CGLN- Helicity- and Invariant Amplitudes
The following relations between CGLN amplitudes and helicity amplitudes will be used in our calculations. (click here for a larger image)

Further details can be found in D. Drechsel and L. Tiator , J. Phys. G 18 (1992) 449-497 (scanned version)
For the Invariant Amplitudes A1,...,A6 we use the definition of F. Berends et al. Nucl. Phys. B4 (1967) 1


Channel: (pi0,p) (pi0,n) (pi+,n) (pi-,p)
Amplitudes: CGLN(F1,...,F6) Helicity(H1,...,H6) Invariant(A1,...,A6)
Choose kinematical variables

choose an independent (running) variable: Q² Q
choose values for Q², W, Q, step size and maximum value:
Q² (GeV/c)²
W (MeV)
Q (deg)
increment
upper value
click here

Change of model parameters:

O(q3) (all couplings in GeV-2)
0
+
-
d9
d8
d20
d21
O(q4) (all couplings in GeV-3)
Isospin 0
e48
e49
e50
e51
e52
e53
e112

Isospin +
e67
e68
e69
e71
e72
e73
e113
Isospin -
e70

Back to Pion Electroproduction Main Page